11.4 - rf-SQUID à jonction π

2020 ◽  
pp. 313-314
Keyword(s):  
2020 ◽  
Vol 2 (2) ◽  
Author(s):  
C. Guarcello ◽  
R. Citro ◽  
O. Durante ◽  
F. S. Bergeret ◽  
A. Iorio ◽  
...  
Keyword(s):  

2007 ◽  
Vol 21 (19) ◽  
pp. 1261-1270 ◽  
Author(s):  
YING-HUA JI ◽  
JU-JU HU ◽  
SHI-HUA CAI

We investigate the relation between the speed of quantum NOT gate and the asymmetry or detuning of the potential in system of the interaction of a two-level rf-SQUID qubit with a classical microwave pulse. The rf-SQUID is characterized by an asymmetric double well potential that gives rise to diagonal matrix elements. Then in resonance, we compare the gate speeds for three-level and two-level quantum NOT gates. We show that in general, a three-level gate is much faster than the conventional two-level gate.


2007 ◽  
Vol 20 (11) ◽  
pp. S445-S449 ◽  
Author(s):  
Douglas A Bennett ◽  
Luigi Longobardi ◽  
Vijay Patel ◽  
Wei Chen ◽  
James E Lukens
Keyword(s):  

2003 ◽  
Vol 29 (2) ◽  
pp. 155-158 ◽  
Author(s):  
S. S. Khvostov ◽  
V. P. Timofeev ◽  
A. S. Garbuz ◽  
V. I. Shnyrkov
Keyword(s):  
High Tc ◽  

2003 ◽  
Vol 52 (10) ◽  
pp. 2580
Author(s):  
Liu Xin-Yuan ◽  
Xie Fei-Xiang ◽  
Meng Shu-Chao ◽  
Ma Ping ◽  
Yang Tao ◽  
...  

PIERS Online ◽  
2009 ◽  
Vol 5 (1) ◽  
pp. 26-30 ◽  
Author(s):  
George P. Tsironis ◽  
N. Lazarides ◽  
M. Eleftheriou
Keyword(s):  

2011 ◽  
Vol 301-303 ◽  
pp. 1705-1709
Author(s):  
Li Xin Xia ◽  
Qian Zhao Lei

We propose a scheme for realizing quantum three-qubit phase gate operation, in a three-mode cavity where the large detuned cavity-mode fields interact with the four-level artificial atom of an rf-SQUID in tripod-type configuration. In this scheme, the two lowest levels of the artificial atom represent the two logical states of the target qubit and two cavity-mode states are the control qubits, while the third cavity-mode field serves the gate manipulation. Since only the metastable lower levels are involved in the gate operations, the gate is insensitive to the decay rates of the artificial atom, which makes this scheme advantageous and it is important in view of decoherence.


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